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power spectral density of digitally modulated signals
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Power Spectral Density of Digitally Modulated Signals Saravanan - - PowerPoint PPT Presentation

Power Spectral Density of Digitally Modulated Signals Saravanan Vijayakumaran sarva@ee.iitb.ac.in Department of Electrical Engineering Indian Institute of Technology Bombay August 22, 2013 1 / 22 PSD Definition for Digitally Modulated


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SLIDE 1

Power Spectral Density of Digitally Modulated Signals

Saravanan Vijayakumaran sarva@ee.iitb.ac.in

Department of Electrical Engineering Indian Institute of Technology Bombay

August 22, 2013

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SLIDE 2

PSD Definition for Digitally Modulated Signals

  • Consider a real binary PAM signal

u(t) =

  • n=−∞

bng(t − nT) where bn = ±1 with equal probability and g(t) is a baseband pulse of duration T

  • PSD = F [Ru(τ)] Neither SSS nor WSS

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SLIDE 3

Cyclostationary Random Process

Definition (Cyclostationary RP)

A random process X(t) is cyclostationary with respect to time interval T if it is statistically indistinguishable from X(t − kT) for any integer k.

Definition (Wide Sense Cyclostationary RP)

A random process X(t) is wide sense cyclostationary with respect to time interval T if the mean and autocorrelation functions satisfy mX(t) = mX(t − T) for all t, RX(t1, t2) = RX(t1 − T, t2 − T) for all t1, t2.

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SLIDE 4

Power Spectral Density of a Cyclostationary Process

To obtain the PSD of a cyclostationary process with period T

  • Calculate autocorrelation of cyclostationary process RX(t, t − τ)
  • Average autocorrelation between 0 and T, RX(τ) = 1

T

T

0 RX(t, t − τ) dt

  • Calculate Fourier transform of averaged autocorrelation RX(τ)

4 / 22

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SLIDE 5

Power Spectral Density of a Realization

Time windowed realizations have finite energy xTo(t) = x(t)I[− To

2 , To 2 ](t)

STo(f) = F(xTo(t)) ˆ Sx(f) = |STo(f)|2 To (PSD Estimate)

PSD of a realization

¯ Sx(f) = lim

To→∞

|STo(f)|2 To |STo(f)|2 To − ⇀ ↽ − 1 To

  • To

2

− To

2

xTo(u)x∗

To(u − τ) du = ˆ

Rx(τ)

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SLIDE 6

Power Spectral Density of a Cyclostationary Process

X(t)X ∗(t − τ) ∼ X(t + T)X ∗(t + T − τ) for cyclostationary X(t) ˆ Rx(τ) = 1 To

  • To

2

− To

2

x(t)x∗(t − τ) dt = 1 KT

  • KT

2

− KT

2

x(t)x∗(t − τ) dt for To = KT = 1 T T 1 K

K 2

  • k=− K

2

x(t + kT)x∗(t + kT − τ) dt − →

K→∞

1 T T E [X(t)X ∗(t − τ)] dt = 1 T T RX(t, t − τ) dt = RX(τ) PSD of a cyclostationary process = F[RX(τ)]

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SLIDE 7

PSD of a Linearly Modulated Signal

  • Consider

u(t) =

  • n=−∞

bnp(t − nT)

  • u(t) is cyclostationary wrt to T if {bn} is stationary
  • u(t) is wide sense cyclostationary wrt to T if {bn} is WSS
  • Suppose Rb[k] = E[bnb∗

n−k]

  • Let Sb(z) = ∞

k=−∞ Rb[k]z−k

  • The PSD of u(t) is given by

Su(f) = Sb

  • e j2πfT |P(f)|2

T

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SLIDE 8

PSD of a Linearly Modulated Signal

Ru(τ) = 1 T T Ru(t + τ, t) dt = 1 T T

  • n=−∞

  • m=−∞

E [bnb∗

mp(t − nT + τ)p∗(t − mT)] dt

= 1 T

  • k=−∞

  • m=−∞

−(m−1)T

−mT

E [bm+kb∗

mp(λ − kT + τ)p∗(λ)] dλ

= 1 T

  • k=−∞

−∞

E [bm+kb∗

mp(λ − kT + τ)p∗(λ)] dλ

= 1 T

  • k=−∞

Rb[k] ∞

−∞

p(λ − kT + τ)p∗(λ) dλ

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SLIDE 9

PSD of a Linearly Modulated Signal

Ru(τ) = 1 T

  • k=−∞

Rb[k] ∞

−∞

p(λ − kT + τ)p∗(λ) dλ ∞

−∞

p(λ + τ)p∗(λ) dλ − ⇀ ↽ − |P(f)|2 ∞

−∞

p(λ − kT + τ)p∗(λ) dλ − ⇀ ↽ − |P(f)|2e −j2πfkT Su(f) = F [Ru(τ)] = |P(f)|2 T

  • k=−∞

Rb[k]e −j2πfkT = Sb

  • e j2πfT |P(f)|2

T where Sb(z) = ∞

k=−∞ Rb[k]z−k. 9 / 22

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SLIDE 10

Power Spectral Density of Line Codes

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SLIDE 11

Line Codes

1 1 1 1 1 1 1 Unipolar NRZ Polar NRZ Bipolar NRZ Manchester

Further reading: Digital Communications, Simon Haykin, Chapter 6

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SLIDE 12

Unipolar NRZ

  • Symbols independent and equally likely to be 0 or A

P (b[n] = 0) = P (b[n] = A) = 1 2

  • Autocorrelation of b[n] sequence

Rb[k] =     

A2 2

k = 0

A2 4

k = 0

  • p(t) = I[0,T)(t) ⇒ P(f) = Tsinc(fT)e −jπfT
  • Power Spectral Density

Su(f) = |P(f)|2 T

  • k=−∞

Rb[k]e −j2πkfT

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SLIDE 13

Unipolar NRZ

Su(f) = A2T 4 sinc2(fT) + A2T 4 sinc2(fT)

  • k=−∞

e −j2πkfT = A2T 4 sinc2(fT) + A2 4 sinc2(fT)

  • n=−∞

δ

  • f − n

T

  • =

A2T 4 sinc2(fT) + A2 4 δ(f)

13 / 22

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SLIDE 14

Normalized PSD plot

0.5 1 1.5 2 0.5 1 fT

Su(f) A2T

Unipolar NRZ

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SLIDE 15

Polar NRZ

  • Symbols independent and equally likely to be −A or A

P (b[n] = −A) = P (b[n] = A) = 1 2

  • Autocorrelation of b[n] sequence

Rb[k] =    A2 k = 0 k = 0

  • P(f) = Tsinc(fT)e −jπfT
  • Power Spectral Density

Su(f) = A2Tsinc2(fT)

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SLIDE 16

Normalized PSD plots

0.5 1 1.5 2 0.5 1 fT

Su(f) A2T

Unipolar NRZ Polar NRZ

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SLIDE 17

Manchester

  • Symbols independent and equally likely to be −A or A

P (b[n] = −A) = P (b[n] = A) = 1 2

  • Autocorrelation of b[n] sequence

Rb[k] =    A2 k = 0 k = 0

  • P(f) = jTsinc

fT

2

  • sin

πfT

2

  • e−jπfT
  • Power Spectral Density

Su(f) = A2Tsinc2 fT 2

  • sin2

πfT 2

  • 17 / 22
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SLIDE 18

Normalized PSD plots

0.5 1 1.5 2 0.5 1 fT

Su(f) A2T

Unipolar NRZ Polar NRZ Manchester

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Bipolar NRZ

  • Successive 1’s have alternating polarity

→ Zero amplitude 1 → +A or − A

  • Probability mass function of b[n]

P (b[n] = 0) = 1 2 P (b[n] = −A) = 1 4 P (b[n] = A) = 1 4

  • Symbols are identically distributed but they are not independent

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SLIDE 20

Bipolar NRZ

  • Autocorrelation of b[n] sequence

Rb[k] =    A2/2 k = 0 − A2/4 k = ±1

  • therwise
  • Power Spectral Density

Su(f) = Tsinc2(fT) A2 2 − A2 4

  • e j2πfT + e −j2πfT

= A2T 2 sinc2(fT) [1 − cos(2πfT)] = A2Tsinc2(fT) sin2(πfT)

20 / 22

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SLIDE 21

Normalized PSD plots

0.5 1 1.5 2 0.5 1 fT

Su(f) A2T

Unipolar NRZ Polar NRZ Manchester Bipolar NRZ

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Thanks for your attention

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